JPH03241782A - Electrostrictive effect element - Google Patents

Electrostrictive effect element

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Publication number
JPH03241782A
JPH03241782A JP2038933A JP3893390A JPH03241782A JP H03241782 A JPH03241782 A JP H03241782A JP 2038933 A JP2038933 A JP 2038933A JP 3893390 A JP3893390 A JP 3893390A JP H03241782 A JPH03241782 A JP H03241782A
Authority
JP
Japan
Prior art keywords
internal electrodes
electrostrictive effect
electrostrictive
effect element
electrodes
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP2038933A
Other languages
Japanese (ja)
Inventor
Yoshiki Inoue
芳樹 井上
Kaneo Uehara
上原 兼雄
Atsushi Ochi
篤 越智
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
NEC Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Corp filed Critical NEC Corp
Priority to JP2038933A priority Critical patent/JPH03241782A/en
Publication of JPH03241782A publication Critical patent/JPH03241782A/en
Pending legal-status Critical Current

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  • General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は電歪効果素子の構造に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to the structure of an electrostrictive element.

〔従来の技術〕[Conventional technology]

電歪効果素子とは、固体の電歪効果を利用して、電気エ
ネルギを機械エネルギに変換するトランスデユーサであ
る。具体的には電歪効果の大きな固体の対向する表面に
金属膜などの電極を形成し、電極間に電位差を与えたと
きに発生する固体の歪を利用している。電界と平行方向
に発生する歪(縦効果歪)は垂直方向に生じる歪(横効
果歪〉より一般には大きいので、前者を利用する方がエ
ネルギ変換効率が高い。このエネルギ変換効率の高い縦
効果を利用した電歪効果素子では、電界強度が大きくな
るほど発生する歪が大きくなるため、大きな変位量を得
るには電界強度が低下しないように印加電圧を大きくす
ることが必要である。しかし、電圧を大きくするために
は大型でかつ高価な電源が必要になり、取扱いに対する
危険度も増す。
An electrostrictive element is a transducer that converts electrical energy into mechanical energy by utilizing the electrostrictive effect of a solid state. Specifically, electrodes such as metal films are formed on opposing surfaces of a solid that has a large electrostrictive effect, and the strain in the solid that occurs when a potential difference is applied between the electrodes is utilized. Since the strain that occurs in the direction parallel to the electric field (longitudinal effect strain) is generally larger than the strain that occurs in the perpendicular direction (transverse effect strain), energy conversion efficiency is higher when using the former.This longitudinal effect, which has high energy conversion efficiency, In an electrostrictive effect element that utilizes a Increasing the size requires a large and expensive power source, which also increases the risk of handling.

このような欠点を改善するために、第4図(a)、(b
)に示すような積層チップコンデンサ型の構造が提案さ
れている。図において、電歪材料1の内部に内部電極2
a、2bが一定の間隔で形成されており、一つおきに外
部電極3a、3bと相互接続している。内部電極2a、
2bの間隔は通常の積層チップコンデンサの技術で数1
0μm程度にすることができる。この構造を採用すると
電極間距離が狭くなるため低電圧で駆動可能な縦効果利
用の電歪効果素子が実現できる。
In order to improve such defects, the
) has been proposed as a multilayer chip capacitor type structure. In the figure, an internal electrode 2 is placed inside the electrostrictive material 1.
electrodes a and 2b are formed at regular intervals, and every other electrode is interconnected with external electrodes 3a and 3b. internal electrode 2a,
The spacing between 2b is several 1 using normal multilayer chip capacitor technology.
The thickness can be set to about 0 μm. If this structure is adopted, the distance between the electrodes becomes narrower, so an electrostrictive effect element using the longitudinal effect that can be driven at a low voltage can be realized.

ところで、積層方向からみた第4図(b)の投影図から
明らかなように、この構造では内部電極の重なる面積(
中央の矩形部分)が素子の断面積と比較して小さい。従
って、基本的には内部電極の重なった部分は電界に応じ
て変形するが、他の部分は変形せず、このため高い電圧
を印加して大きな歪を発生させると変形する部分と変形
しにくい部分との境界に大きな応力の集中が起こり、素
子が機械的に破壊する欠点がある。
By the way, as is clear from the projection view of FIG. 4(b) viewed from the stacking direction, in this structure, the overlapping area of the internal electrodes (
The central rectangular portion) is small compared to the cross-sectional area of the element. Therefore, basically, the overlapping part of the internal electrodes deforms in response to the electric field, but the other parts do not. Therefore, when a high voltage is applied and a large strain is generated, some parts deform and are difficult to deform. There is a drawback that a large stress concentration occurs at the boundary between the parts and the element is mechanically destroyed.

このような従来素子の欠点を改善するために、積層チッ
プコンデンサ型構造の電歪効果素子について、第5図に
示すように、その積層方向に平行な側面上に各内部電極
に平行に溝(以下スリットという)6を形成する構造が
ある(特開昭58−196077)。すなわち、素子の
積層方向に垂直な断面において素子の変形に関与しない
周辺部の一部を取り除くことにより応力集中を緩和させ
て、電圧の繰返しパルス印加に対して機械的破壊に至る
までの寿命を伸ばし、さらに素子の変位も増大させるこ
とができる。
In order to improve these drawbacks of conventional elements, grooves ( There is a structure that forms a slit (hereinafter referred to as a slit) (Japanese Patent Application Laid-Open No. 58-196077). In other words, in a cross section perpendicular to the stacking direction of the device, by removing a part of the periphery that is not involved in deformation of the device, stress concentration is alleviated, thereby increasing the lifespan until mechanical failure occurs under repeated voltage pulse application. In addition, the displacement of the element can be increased.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上述した従来の電歪効果素子の問題点について、図面を
用いて説明する。
The problems of the conventional electrostrictive effect element described above will be explained with reference to the drawings.

第6図(a)は、従来の電歪効果素子の縦断面図、第6
図(b)、(c)はそれぞれスリット形状5と、内部電
極2a、2b、2c、2dとを、素子の積層方向と垂直
な面に投影した図である。
FIG. 6(a) is a vertical cross-sectional view of a conventional electrostrictive effect element.
Figures (b) and (c) are diagrams in which the slit shape 5 and the internal electrodes 2a, 2b, 2c, and 2d are projected onto a plane perpendicular to the stacking direction of the element.

スリット6をはさんだ位置にある二枚の内部電極2c、
2dはそれぞれ異なる外部電極3a、3bに接続してい
る。従って、外部型ftl1!3 aと3b間に電圧を
印加すると、内部電極2Cと2d間には電界が生ずる。
two internal electrodes 2c located across the slit 6;
2d are connected to different external electrodes 3a and 3b, respectively. Therefore, when a voltage is applied between the external type ftl1!3a and 3b, an electric field is generated between the internal electrodes 2C and 2d.

このときの電気力線の分布は、第7図のように示される
。電歪効果素子では、変位量は電界強度の増大に伴って
大きくなるが、第7図のように、この構造の電歪効果素
子はスリット6の先端に電界が集中するために、大きい
変位量を取り出す目的で高い電圧を印加すると、その部
分で絶縁破壊が起りやすい。このように従来の構造では
、絶縁破壊を生じさせないように印加電圧を低く抑える
必要があるため、大きな変位量を取り出せないという欠
点がある。
The distribution of electric lines of force at this time is shown as shown in FIG. In an electrostrictive effect element, the amount of displacement increases as the electric field strength increases, but as shown in FIG. If a high voltage is applied to extract the material, dielectric breakdown is likely to occur at that part. As described above, the conventional structure has the disadvantage that a large amount of displacement cannot be obtained because the applied voltage must be kept low so as not to cause dielectric breakdown.

本発明の目的は、このような欠点を除きスリットをはさ
む2枚の内部電極を同一の外部電極に接続することによ
り、スリット先端への電界集中をさけ、絶縁破壊を起り
に<<シて大きな変位量を取出せるようにした電歪効果
素子を提供することにある。
The purpose of the present invention is to eliminate such drawbacks and connect the two internal electrodes that sandwich the slit to the same external electrode, thereby avoiding concentration of electric field at the tip of the slit and preventing dielectric breakdown from occurring. An object of the present invention is to provide an electrostrictive effect element capable of extracting a displacement amount.

〔課題を解決するための手段〕[Means to solve the problem]

本発明の槽底は、電歪効果を示す材料と内部電極とが交
互に積層されこれら内部電極が二つの外部電極のどちら
かに接続されると共に、これら素子の積層方向と平行な
側面上に、前記内部電極の電極面と平行に所定の間隔で
溝が一箇所以上に形成されて構成される電歪効果素子に
おいて、前記の多溝を挟む2枚の内部電極が、同一の外
部電極に接続されていることを特徴とする。
In the tank bottom of the present invention, materials exhibiting an electrostrictive effect and internal electrodes are alternately laminated, and these internal electrodes are connected to one of two external electrodes, and on the side surface parallel to the lamination direction of these elements. , in an electrostrictive effect element in which grooves are formed at one or more places parallel to the electrode surface of the internal electrode at predetermined intervals, two internal electrodes sandwiching the multi-grooves are formed on the same external electrode; It is characterized by being connected.

また、本発明において.各溝を挟む2枚の内部電極の間
の間隔が、他の内部電極の間の間隔よりも狭くしたもの
とすることもできる。
Moreover, in the present invention. The distance between the two internal electrodes sandwiching each groove may be narrower than the distance between the other internal electrodes.

〔実施例〕〔Example〕

次に本発明について図面を参照にして説明する。 Next, the present invention will be explained with reference to the drawings.

第1図(a>、(b)、(c)は本発明の一実施例の構
造を示す電歪効果素子の縦断面図、およびそのスリット
形状5および内部電極2a〜2hを素子の積層方向と垂
直な面に投影した図である。スリット6をはさんだ位置
にある内部電極2eと2fはどちらも外部電極3aに接
続し、同様に内部電極2gと2hはどちらも外部電極3
bに接続している。従って、外部電極3a、3bに電圧
を印加しても、スリット6のある層には電界が5− 6− 生じない。
FIGS. 1(a), (b), and (c) are longitudinal cross-sectional views of an electrostrictive element showing the structure of an embodiment of the present invention, and the slit shape 5 and internal electrodes 2a to 2h are shown in the stacking direction of the element. The internal electrodes 2e and 2f located across the slit 6 are both connected to the external electrode 3a, and similarly the internal electrodes 2g and 2h are both connected to the external electrode 3.
connected to b. Therefore, even if a voltage is applied to the external electrodes 3a and 3b, no electric field is generated in the layer where the slit 6 is located.

本実施例では、電歪効果素子の横断面を4×4IllI
ll、内部電極2a、2e、2fと2b、2g。
In this example, the cross section of the electrostrictive element is 4×4IllI
ll, internal electrodes 2a, 2e, 2f and 2b, 2g.

2hとの重なる部分を3×3印、スリット形状5は3×
3■とした。また、素子高さは10mm、スリット6の
配置間隔は約0.5++++n、電圧のかかる内部電極
間の配置間隔は約100μm、内部電極2eと2f問お
よび2gと2h間の間隔、すなわちスリット6のある層
の厚みは約200μmとした。内部電極2a、2b、2
e〜2hは総数で80枚形形成た。本実施例の素子は、
スリット6のある層は電圧がかからないために変位は生
じず、従って本実施例では変位の生じる層(以下機能層
という)は60層である。
The part that overlaps with 2h is marked 3x3, and the slit shape 5 is 3x
It was set as 3■. The element height is 10 mm, the spacing between the slits 6 is about 0.5++++n, the spacing between the internal electrodes to which voltage is applied is about 100 μm, and the spacing between the internal electrodes 2e and 2f and between 2g and 2h, that is, the spacing between the slits 6 The thickness of one layer was approximately 200 μm. Internal electrodes 2a, 2b, 2
A total of 80 sheets were formed for e to 2h. The device of this example is
Since no voltage is applied to the layer with the slit 6, no displacement occurs; therefore, in this embodiment, there are 60 layers (hereinafter referred to as functional layers) in which displacement occurs.

本実施例の具体例として、チタン酸ジルコン酸鉛系の電
歪効果を示す材料を用いて調べた。本材料の予焼粉末に
有機系の溶剤、バインダ、可塑材を添加して、ドクター
・ブレード法で約130μmの厚さのグリーンシートを
作製した。このグリーンシートを乾燥したのち、その上
に銀−パラジウム合金粉末を主成分とする内部電極用ペ
ーストと、カーボンを主成分とするスリット用空孔形成
材ペーストとを所定枚数スクリーン印刷し、所定の形状
に切断して積層、熱圧着した。これを1100℃で焼成
した。この昇温の際に空孔形成材が飛散す・ることによ
り、スリット6が形成される。この焼成後、外部電極用
Agペーストを焼き付けた後、電圧印加用のリード線を
接続した。
As a specific example of this example, a lead zirconate titanate material exhibiting an electrostrictive effect was used for investigation. An organic solvent, a binder, and a plasticizer were added to the pre-fired powder of this material, and a green sheet with a thickness of about 130 μm was produced using a doctor blade method. After drying this green sheet, a predetermined number of sheets of internal electrode paste containing silver-palladium alloy powder as a main component and slit pore forming material paste containing carbon as a main component are screen printed on it. They were cut into shapes, laminated, and bonded under heat. This was fired at 1100°C. The slits 6 are formed by scattering the pore-forming material during this temperature rise. After this firing, the Ag paste for external electrodes was baked, and then lead wires for voltage application were connected.

本実施例による電歪効果素子と、内部電極の配置のみ異
なる従来i造の電歪効果素子(機能層は79層になる)
について、それぞれ20個ずつ、150VDCで1分間
の分極処理を施した後、100VDC/min、の昇圧
速度で電圧を印加した場合の変位の変化を調査した。結
果を第2図のグラフに示す。従来構造の素子では、28
0十4O−50Vで絶縁破壊を起したのに対し、本発明
による素子では、700Vでも絶縁破壊は生じなかった
。その結果、従来構造の素子に較べて大きな変位量が得
られた。
The electrostrictive effect element according to this embodiment and the conventional i-structured electrostrictive effect element that differs only in the arrangement of internal electrodes (79 functional layers)
After 20 pieces of each were polarized at 150 VDC for 1 minute, changes in displacement were investigated when voltage was applied at a boost rate of 100 VDC/min. The results are shown in the graph of FIG. In an element with a conventional structure, 28
In contrast, dielectric breakdown occurred at 014O-50V, whereas dielectric breakdown did not occur even at 700V in the element according to the present invention. As a result, a larger amount of displacement was obtained compared to elements with conventional structures.

第3図は本発明の第2の実施例の電歪効果素子の縦断面
図である。スリット6をはさんだ位置にある内部電極2
eと2f間または内部電極2gと2hの間には電圧が加
わらないために、この部分の電極間距離を短くしても絶
縁破壊が生じない。
FIG. 3 is a longitudinal sectional view of an electrostrictive element according to a second embodiment of the present invention. Internal electrode 2 located across slit 6
Since no voltage is applied between e and 2f or between internal electrodes 2g and 2h, no dielectric breakdown occurs even if the distance between the electrodes in this area is shortened.

本実施例では、内部電極間を50μmとした。また、ス
リット6自体の厚みは約5μmである。素子高さは10
IIIa、電圧のかかる内部電極間の距離は約100μ
mと、いずれも第1の実施例と同じ寸法とした。内部電
極2a、 2b、 2e〜2hは総数で11枚形形成た
。
In this example, the distance between the internal electrodes was 50 μm. Further, the thickness of the slit 6 itself is approximately 5 μm. The element height is 10
IIIa, the distance between internal electrodes to which voltage is applied is approximately 100μ
m, both have the same dimensions as in the first embodiment. A total of 11 internal electrodes 2a, 2b, 2e to 2h were formed.

本実施例の素子の機能層数は84層となる。他の寸法は
第1の実施例に一致させた。第1の実施例と同条件で電
圧を印加した場合の、変位の変化について調査した結果
を第2図の特性図に示す。
The number of functional layers in the device of this example is 84. Other dimensions were consistent with the first example. The characteristic diagram in FIG. 2 shows the results of investigating changes in displacement when voltage was applied under the same conditions as in the first embodiment.

本実施例では、従来構造素子よりも電圧−変位効率の高
い素子が得られ、また、本実施例の20個の素子につい
て電圧を印加したがいずれも700■では絶縁破壊が生
じなかった。
In this example, an element having a higher voltage-displacement efficiency than the conventional structural element was obtained, and when a voltage was applied to 20 elements of this example, no dielectric breakdown occurred at 700 .mu.m.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明によれば、スリットをはさむ
位置にある2枚の内部電極が、同一の外部電極に接続し
ている構造とすることにより、高い電圧を印加したとき
の絶縁破壊を防止することができるために、絶縁破壊電
圧が高く、かつ、より大きな変位量を取り出すことので
きる構造の電歪効果素子が得られる、という効果がある
。
As explained above, according to the present invention, two internal electrodes sandwiching a slit are connected to the same external electrode, thereby preventing dielectric breakdown when high voltage is applied. Therefore, there is an effect that an electrostrictive effect element having a structure that has a high dielectric breakdown voltage and can extract a larger amount of displacement can be obtained.

【図面の簡単な説明】[Brief explanation of drawings]

第1図(a)は本発明の一実施例の電歪効果素子の縦断
面図、第1図(b)、(C)は第1図のスリット形状5
と、内部電極2を素子の積層方向と垂直な面に投影した
図、第2図は電圧を印加した場合の変位の変化を示した
特性図、第3図は本発明の第2の実施例の縦断面図、第
4図(a)。 (b)は従来の積層チップコンデンサ構造の素子の縦断
面図、およびその内部電極2の投影図、第5図は従来例
の素子の断面図、第6図(a〉。 (b)、(C)は従来構造の素子の縦断面図およびその
スリット形状5と内部電極2a、2bの投影図、第7図
は従来例の素子の電気力線の分布を9− 10− 示した模式図である。 1・・・電歪材料、2a〜2h・・・内部電極、3a。 3b・・・外部電極、4・・・リード線、5・・・スリ
ット形状、6・・・スリット。
FIG. 1(a) is a vertical cross-sectional view of an electrostrictive effect element according to an embodiment of the present invention, and FIGS. 1(b) and (C) are slit shapes 5 of FIG.
FIG. 2 is a characteristic diagram showing the change in displacement when voltage is applied, and FIG. 3 is a diagram showing the second embodiment of the present invention. A vertical cross-sectional view of FIG. 4(a). (b) is a vertical cross-sectional view of an element with a conventional multilayer chip capacitor structure and a projected view of its internal electrode 2, FIG. 5 is a cross-sectional view of a conventional element, and FIG. 6 (a). C) is a longitudinal cross-sectional view of an element with a conventional structure and a projected view of its slit shape 5 and internal electrodes 2a, 2b, and FIG. 7 is a schematic diagram showing the distribution of electric lines of force in the element of the conventional example. 1... Electrostrictive material, 2a to 2h... Internal electrode, 3a. 3b... External electrode, 4... Lead wire, 5... Slit shape, 6... Slit.

Claims (2)

【特許請求の範囲】[Claims] 1.電歪効果を示す材料と内部電極とが交互に積層され
これら内部電極が二つの外部電極のどちらかに接続され
ると共に、これら素子の積層方向と平行な側面上に、前
記内部電極の電極面と平行に所定の間隔で溝が一箇所以
上に形成されて構成される電歪効果素子において、前記
の各溝を挟む2枚の内部電極が、同一の外部電極に接続
されていることを特徴とする電歪効果素子。
1. Materials exhibiting an electrostrictive effect and internal electrodes are alternately laminated, and these internal electrodes are connected to either of the two external electrodes, and the electrode surface of the internal electrode is placed on the side surface parallel to the lamination direction of these elements. An electrostrictive effect element comprising one or more grooves formed at a predetermined interval in parallel with the grooves, characterized in that two internal electrodes sandwiching each groove are connected to the same external electrode. An electrostrictive effect element.
2.各溝を挟む2枚の内部電極の間の間隔が、他の内部
電極の間の間隔よりも狭くしたものである請求項1記載
の電歪効果素子。
2. 2. The electrostrictive effect element according to claim 1, wherein the distance between the two internal electrodes sandwiching each groove is narrower than the distance between the other internal electrodes.
JP2038933A 1990-02-19 1990-02-19 Electrostrictive effect element Pending JPH03241782A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2038933A JPH03241782A (en) 1990-02-19 1990-02-19 Electrostrictive effect element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2038933A JPH03241782A (en) 1990-02-19 1990-02-19 Electrostrictive effect element

Publications (1)

Publication Number Publication Date
JPH03241782A true JPH03241782A (en) 1991-10-28

Family

ID=12539031

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2038933A Pending JPH03241782A (en) 1990-02-19 1990-02-19 Electrostrictive effect element

Country Status (1)

Country Link
JP (1) JPH03241782A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006216850A (en) * 2005-02-04 2006-08-17 Tdk Corp Multilayer piezoelectric element
US8240582B2 (en) 2007-02-26 2012-08-14 Denso Corporation Stacked piezoelectric device

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61174681A (en) * 1985-01-28 1986-08-06 Sony Corp Manufacture of laminated piezoelectric device
JPS63102384A (en) * 1986-10-20 1988-05-07 Fuji Electric Co Ltd Laminated piezoelectric actuator device
JPH0258385A (en) * 1988-08-24 1990-02-27 Murata Mfg Co Ltd electrostrictive actuator

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61174681A (en) * 1985-01-28 1986-08-06 Sony Corp Manufacture of laminated piezoelectric device
JPS63102384A (en) * 1986-10-20 1988-05-07 Fuji Electric Co Ltd Laminated piezoelectric actuator device
JPH0258385A (en) * 1988-08-24 1990-02-27 Murata Mfg Co Ltd electrostrictive actuator

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006216850A (en) * 2005-02-04 2006-08-17 Tdk Corp Multilayer piezoelectric element
US8240582B2 (en) 2007-02-26 2012-08-14 Denso Corporation Stacked piezoelectric device

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